The large-N limit of the 4d N $$ \mathcalN} $$ = 1 superconformal index

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Location: Deutsche Nationalbibliothek Frankfurt am Main

ISSN: 1029-8479

Extent: Online-Ressource

Language: Englisch

Notes: online resource.

Bibliographic citation: The large-N limit of the 4d N $$ \mathcalN} $$ = 1 superconformal index ; volume:2020 ; number:11 ; day:27 ; month:11 ; year:2020 ; pages:1-59 ; date:11.2020
Journal of high energy physics ; 2020, Heft 11 (27.11.2020), 1-59, 11.2020

Creator: Cabo-Bizet, Alejandro
Cassani, Davide
Martelli, Dario
Murthy, Sameer

Contributor: SpringerLink (Online service)

DOI: 10.1007/JHEP11(2020)150

URN: urn:nbn:de:101:1-2021010721522055472188

Rights: Open Access; Der Zugriff auf das Objekt ist unbeschränkt möglich.

Last update: 15.08.2025, 7:22 AM CEST

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Cabo-Bizet, Alejandro
Cassani, Davide
Martelli, Dario
Murthy, Sameer
SpringerLink (Online service)

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The large-N limit of the 4d N $$ \mathcalN} $$ = 1 superconformal index

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Other Objects (12)

Residues, modularity, and the Cardy limit of the 4d N $$ \mathcalN} $$ = 4 superconformal index

BPS index and 4d N $$ \mathcalN} $$ = 2 superconformal field theories

S-folds and 4d N $$ \mathcalN} $$ = 3 superconformal field theories

On 4d rank-one N = 3 $$ \mathcalN}=3 $$ superconformal field theories

A new 4d N $$ \mathcalN} $$ = 1 duality from the superconformal index

The planar limit of N $$ \mathcalN} $$ = 2 superconformal field theories

The planar limit of N $$ \mathcalN} $$ = 2 superconformal quiver theories

R-current three-point functions in 4d N $$ \mathcalN} $$ = 1 superconformal theories

Bootstrapping N = 3 $$ \mathcalN}=3 $$ superconformal theories

The N = 2 $$ \mathcalN}=2 $$ superconformal bootstrap

Revisiting N = 4 $$ \mathcalN}=4 $$ superconformal blocks

Microstate counting via Bethe Ansätze in the 4d N $$ \mathcalN} $$ = 1 superconformal index

Residues, modularity, and the Cardy limit of the 4d N $$ \mathcalN} $$ = 4 superconformal index

BPS index and 4d N $$ \mathcalN} $$ = 2 superconformal field theories

S-folds and 4d N $$ \mathcalN} $$ = 3 superconformal field theories

On 4d rank-one N = 3 $$ \mathcalN}=3 $$ superconformal field theories

A new 4d N $$ \mathcalN} $$ = 1 duality from the superconformal index

The planar limit of N $$ \mathcalN} $$ = 2 superconformal field theories

The planar limit of N $$ \mathcalN} $$ = 2 superconformal quiver theories

R-current three-point functions in 4d N $$ \mathcalN} $$ = 1 superconformal theories

Bootstrapping N = 3 $$ \mathcalN}=3 $$ superconformal theories

The N = 2 $$ \mathcalN}=2 $$ superconformal bootstrap

Revisiting N = 4 $$ \mathcalN}=4 $$ superconformal blocks

Microstate counting via Bethe Ansätze in the 4d N $$ \mathcalN} $$ = 1 superconformal index

Residues, modularity, and the Cardy limit of the 4d N $$ \mathcalN} $$ = 4 superconformal index

BPS index and 4d N $$ \mathcalN} $$ = 2 superconformal field theories

S-folds and 4d N $$ \mathcalN} $$ = 3 superconformal field theories

On 4d rank-one N = 3 $$ \mathcalN}=3 $$ superconformal field theories

A new 4d N $$ \mathcalN} $$ = 1 duality from the superconformal index

The planar limit of N $$ \mathcalN} $$ = 2 superconformal field theories

The planar limit of N $$ \mathcalN} $$ = 2 superconformal quiver theories

R-current three-point functions in 4d N $$ \mathcalN} $$ = 1 superconformal theories

Bootstrapping N = 3 $$ \mathcalN}=3 $$ superconformal theories

The N = 2 $$ \mathcalN}=2 $$ superconformal bootstrap

Revisiting N = 4 $$ \mathcalN}=4 $$ superconformal blocks

Microstate counting via Bethe Ansätze in the 4d N $$ \mathcalN} $$ = 1 superconformal index

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